FIG. 1.—PRINCIPLE OF GALILEAN TELESCOPE.

Galileo's first discoveries with this instrument were made in 1610, and it was not till nearly half a century later that any great improvement in telescopic construction was effected. In the middle of the seventeenth century Scheiner and Huygens made telescopes on the principle, suggested by Kepler, of using two double convex lenses instead of a convex and a concave, and the modern refracting telescope is still constructed on essentially the same principle, though, of course, with many minor modifications (Fig. 2).

FIG. 2.—PRINCIPLE OF COMMON REFRACTOR.

The latter part of the seventeenth century witnessed the introduction of telescopes on this principle of the most amazing length, the increase in length being designed to minimize the imperfections which a simple lens exhibits both in definition and in colour. Huygens constructed one such telescope of 123 feet focal length, which he presented to the Royal Society of London; Cassini, at Paris, used instruments of 100 and 136 feet; while Bradley, in 1722, measured the diameter of Venus with a glass whose focal length was 212¼ feet. Auzout is said to have made glasses of lengths varying from 300 to 600 feet, but, as might have been expected, there is no record of any useful observations having ever been made with these monstrosities. Of course, these instruments differed widely from the compact and handy telescopes with which we are now familiar. They were entirely without tubes. The object-glass was fastened to a tall pole or to some high building, and was painfully manœuvred into line with the eye-piece, which was placed on a support near the ground, by means of an arrangement of cords. The difficulties of observation with these unwieldy monsters must have been of the most exasperating type, while their magnifying power did not exceed that of an ordinary modern achromatic of, perhaps, 36 inches focal length. Cassini, for instance, seems never to have gone beyond a power of 150 diameters, which might be quite usefully employed on a good modern 3-inch refractor in good air. Yet with such tools he was able to discover four of the satellites of Saturn and that division in Saturn's ring which still bears his name. Such facts speak volumes for the quality of the observer. Those who are the most accustomed to use the almost perfect products of modern optical skill will have the best conception of, and the profoundest admiration for, the limitless patience and the wonderful ability which enabled him to achieve such results with the very imperfect means at his disposal.

The clumsiness and unmanageableness of these aerial telescopes quickly reached a point which made it evident that nothing more was to be expected of them; and attempts were made to find a method of combining lenses, which might result in an instrument capable of bearing equal or greater magnifying powers on a much shorter length. The chief hindrance to the efficiency of the refracting telescope lies in the fact that the rays of different colours which collectively compose white light cannot be brought to one focus by any single lens. The red rays, for example, have a different focal length from the blue, and so any lens which brings the one set to a focus leaves a fringe of the other outstanding around any bright object.

In 1729 Mr. Chester Moor Hall discovered a means of conquering this difficulty, but his results were not followed up, and it was left for the optician John Dollond to rediscover the principle some twenty-five years later. By making the object-glass of the telescope double, the one lens being of crown and the other of flint glass, he succeeded in obtaining a telescope which gave a virtually colourless image.

This great discovery of the achromatic form of construction at once revolutionized the art of telescope-making. It was found that instruments of not more than 5 feet focal length could be constructed, which infinitely surpassed in efficiency, as well as in handiness, the cumbrous tools which Cassini had used; and Dollond's 5-foot achromatics, generally with object-glasses of 3¾ inches diameter, represented for a considerable time the acme of optical excellence. Since the time of Dollond, the record of the achromatic refractor has been one of continual, and, latterly, of very rapid progress. For a time much hindrance was experienced from the fact that it proved exceedingly difficult to obtain glass discs of any size whose purity and uniformity were sufficient to enable them to pass the stringent test of optical performance. In the latter part of the eighteenth century, a 6-inch glass was considered with feelings of admiration, somewhat similar to those with which we regard the Yerkes 40-inch to-day; and when, in 1823, the Dorpat refractor of 96⁄10 inches was mounted (Fig. 3), the astronomical world seemed to have the idea that something very like finality had been reached. The Dorpat telescope proved, however, to be only a milestone on the path of progress. Before very long it was surpassed by a glass of 12 inches diameter, which Sir James South obtained from Cauchoix of Paris, and which is now mounted in the Dunsink Observatory, Dublin. This, in its turn, had to give place to the fine instruments of 14·9 inches which were figured by Merz of Munich for the Pulkowa and Cambridge (U.S.A.) Observatories; and then there came a pause of a few years, which was broken by Alvan Clark's completion of an 18½-inch, an instrument which earned its diploma, before ever it left the workshop of its constructor, by the discovery of the companion to Sirius.